Samarium hexaboride

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Samarium hexaboride
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Identifiers
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3D model (JSmol)
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  • InChI=1S/6B.Sm
    Key: IYKQPDWKORWUNW-UHFFFAOYSA-N
  • [B].[B].[B].[B].[B].[B].[Sm]
Properties
B6Sm
Molar mass 215.22 g·mol−1
Melting point 2400 °C ±100[1]
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).

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Samarium hexaboride (SmB6) is an intermediate-valence compound where samarium is present both as Sm2+ and Sm3+ ions at the ratio 3:7.[2] It is a Kondo insulator having a metallic surface state.[3]

Early studies

It was first studied by soviet scientists in the early 1960s.[4] Further studies were then undertaken at Bell Laboratories.[4] By 1968 their researchers had noted changes in the electronic configuration at different temperatures.[5] At temperatures above 50 K its properties are typical of a Kondo metal, with metallic electrical conductivity characterized by strong electron scattering, whereas at low temperatures, it behaves as a non-magnetic insulator with a narrow band gap of about 4–14 meV.[6] The cooling-induced metal-insulator transition in SmB6 is accompanied by a sharp increase in thermal conductivity, peaking at about 15 K. The reason for this increase is that electrons do not contribute to thermal conductivity at low temperatures, which is instead dominated by phonons. The decrease in electron concentration reduced the rate of electron-phonon scattering.[7]

Twenty first century research

By the twenty first century condensed matter physicists grew more interested in Page Module:Chem2/styles.css has no content.SmB6 with claims that it may be a topological insulator.[8][9][10] Other researchers found no evidence of topological surface states.[11]

The increasing electrical resistance with a reduction in temperature indicates that the material behaves as an insulator; however, recent measurements reveal a Fermi surface (an abstract boundary of electrons in momentum space) characteristic of a good metal, indicating a more exotic dual metal-insulating ground state.[12][13] The electrical resistivity at temperatures below 4K displays a distinct plateau,[14] which is thought to be the coexistence of an insulating state (bulk) and a conducting state (surface). At temperatures approaching absolute zero, the quantum oscillations of the material grow as the temperature declines, a behavior that contradicts both the Fermi analysis and the rules that govern conventional metals.[12][15][13] While it has been argued that quantum oscillations on samples grown from aluminium flux[16] may arise from aluminum inclusions,[17] such an explanation is excluded for samples grown by the image furnace method[12][14] rather than by the flux growth method.[16][17]

See also

References

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  1. ^ Plenum Press Handbooks of High-Temperature Materials: No. 1 Materials Index p42
  2. ^ Page Module:Citation/CS1/styles.css has no content.Nickerson, J.; White, R.; Lee, K.; Bachmann, R.; Geballe, T.; Hull, G. (1971). "Physical Properties of SmB6". Physical Review B. 3 (6): 2030. Bibcode:1971PhRvB...3.2030N. doi:10.1103/PhysRevB.3.2030.
  3. ^ Page Module:Citation/CS1/styles.css has no content.Li, Lu; Sun, Kai; Kurdak, Cagliyan; Allen, J. W. (2020). "Emergent mystery in the Kondo insulator samarium hexaboride". Nature Reviews Physics. 2 (9): 463–479. Bibcode:2020NatRP...2..463L. doi:10.1038/s42254-020-0210-8. ISSN 2522-5820. OSTI 1649780. S2CID 257113116.
  4. ^ a b Page Module:Citation/CS1/styles.css has no content.Wolchover, Natalie (2015). "Paradoxical Crystal Baffles Physicists". Quanta Magazine. Retrieved 12 May 2023.
  5. ^ Page Module:Citation/CS1/styles.css has no content.Menth, A.; Buehler, E.; Geballe, T. H. (17 February 1969). "Magnetic and Semiconducting Properties of Sm B 6". Physical Review Letters. 22 (7): 295–297. Bibcode:1969PhRvL..22..295M. doi:10.1103/PhysRevLett.22.295.
  6. ^ Page Module:Citation/CS1/styles.css has no content.Nyhus, P.; Cooper, S.; Fisk, Z.; Sarrao, J. (1995). "Light scattering from gap excitations and bound states in SmB6". Physical Review B. 52 (20): 14308–14311. Bibcode:1995PhRvB..5214308N. doi:10.1103/PhysRevB.52.R14308. PMID 9980746.
  7. ^ Page Module:Citation/CS1/styles.css has no content.Sera, M.; Kobayashi, S.; Hiroi, M.; Kobayashi, N.; Kunii, S. (1996). "Thermal conductivity of RB6 (R=Ce, Pr, Nd, Sm, Gd) single crystals". Physical Review B. 54 (8): R5207–R5210. Bibcode:1996PhRvB..54.5207S. doi:10.1103/PhysRevB.54.R5207. PMID 9986570.
  8. ^ Page Module:Citation/CS1/styles.css has no content.Botimer, J.; Kim; Thomas; Grant; Fisk; Jing Xia (2013). "Robust Surface Hall Effect and Nonlocal Transport in SmB6: Indication for an Ideal Topological Insulator". Scientific Reports. 3: 3150. arXiv:1211.6769. Bibcode:2013NatSR...3.3150K. doi:10.1038/srep03150. PMC 3818682. PMID 24193196.
  9. ^ Page Module:Citation/CS1/styles.css has no content.Xiaohang Zhang; N. P. Butch; P. Syers; S. Ziemak; Richard L. Greene; Johnpierre Paglione (2013). "Hybridization, Inter-Ion Correlation, and Surface States in the Kondo Insulator SmB6". Phys. Rev. X. 3 (1) 011011. arXiv:1211.5532. Bibcode:2013PhRvX...3a1011Z. doi:10.1103/PhysRevX.3.011011. S2CID 53638956.
  10. ^ Page Module:Citation/CS1/styles.css has no content.Wolgast, Steven; Kurdak, Çağlıyan; Sun, Kai; Allen, J. W.; Kim, Dae-Jeong; Fisk, Zachary (2013). "Low-temperature surface conduction in the Kondo insulator SmB6". Phys. Rev. B. 88 (18) 180405. arXiv:1211.5104. Bibcode:2013PhRvB..88r0405W. doi:10.1103/physrevb.88.180405. ISSN 1098-0121. S2CID 119242604.
  11. ^ Page Module:Citation/CS1/styles.css has no content.Hlawenka; Siemensmeyer; Weschke; Varykhalov; Sánchez-Barriga; Shitsevalova; Dukhnenko; Filipov; Gabáni; Flachbart; Rader; Rienks (2018). "Samarium hexaboride is a trivial surface conductor". Nature Communications. 9 (1): 1–7. arXiv:1502.01542. Bibcode:2018NatCo...9..517H. doi:10.1038/s41467-018-02908-7. PMC 5802797. PMID 29410418.
  12. ^ a b c Page Module:Citation/CS1/styles.css has no content.B. S. Tan; Y.-T. Hsu; B. Zeng; M. Ciomaga Hatnean; N. Harrison; Z. Zhu; M. Hartstein; M. Kiourlappou; A. Srivastava; M. D. Johannes; T. P. Murphy; J.-H. Park; L. Balicas; G. G. Lonzarich; G. Balakrishnan; Suchitra Sebastian (2015). "Unconventional Fermi surface in an insulating state". Science. 349 (6245): 287–290. arXiv:1507.01129. Bibcode:2015Sci...349..287T. doi:10.1126/science.aaa7974. PMID 26138105. S2CID 206635941.
  13. ^ a b Page Module:Citation/CS1/styles.css has no content.Natalie Wolchover (2 July 2015). "Paradoxical Crystal Baffles Physicists". Quanta Magazine. Retrieved 2020-01-15.
  14. ^ a b Page Module:Citation/CS1/styles.css has no content.M. Ciomaga Hatnean; M. R. Lees; D. Mck. Paul; G. Balakrishnan (2013). "Large, high quality single-crystals of the new Topological Kondo Insulator, SmB6". Nature. 3 (3071): 3071. Bibcode:2013NatSR...3E3071H. doi:10.1038/srep03071. PMC 3810659. PMID 24166216.
  15. ^ Page Module:Citation/CS1/styles.css has no content.Borghino, Dario (July 7, 2015). "Puzzling material acts as conductor and insulator at the same time". www.gizmag.com. Retrieved 2015-07-08.
  16. ^ a b Page Module:Citation/CS1/styles.css has no content.Li, G.; Xiang, Z.; Yu, F.; Asaba, T.; Lawson, B.; Cai, P.; Tinsman, C.; Berkley, A.; Wolgast, S. (2014-12-05). "Two-dimensional Fermi surfaces in Kondo insulator SmB6". Science. 346 (6214): 1208–1212. arXiv:1306.5221. Bibcode:2014Sci...346.1208L. doi:10.1126/science.1250366. ISSN 0036-8075. PMID 25477456. S2CID 39786801.
  17. ^ a b Page Module:Citation/CS1/styles.css has no content.S. M. Thomas; Xiaxin Ding; F. Ronning; V. Zapf; J. D. Thompson; Z. Fisk; J. Xia; P. F. S. Rosa (2019). "Quantum oscillations in flux-grown SmB6 with embedded aluminum". Physical Review Letters. 122 (16) 166401. arXiv:1806.00117. Bibcode:2019PhRvL.122p6401T. doi:10.1103/PhysRevLett.122.166401. PMID 31075018. S2CID 59407039.

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